Title: Ling Qian Clive Mingham Derek Causon David Ingram
1 Ling Qian Clive Mingham Derek Causon David
Ingram
Numerical Simulation of a Wave Driven Rotating
Vane Using a Two-Fluid Solver
by
of
Centre for Mathematical Modelling and Flow
Analysis, Manchester Metropolitan University, UK
2Acknowledgements
- EPSRC (UK) for funding the project
- Trevor Whittaker and Matt Folley
- Queens University, Belfast, U. K.
3Outline
- Background
- - the wave energy device
- - modelling issues
- Numerics
- Solver
- Gridding
- Results
- Conclusions
4Wave Energy Device
- - is based on the pendular principle.
5Modelling Issues
- Device simulation has to model
- Complex flow including
- wave breaking
- vortex formation
- air entrainment
- Complicated geometry
- Moving solid bodies
6Numerics AMAZON-SC
- Written in-house
- Two fluid, time accurate, conservation law based,
flow code utilising the surface capturing
approach - Cartesian cut cell techniques are used to
represent solid static or moving boundaries
7Governing Equations
- - 2D incompressible, Euler equations with
variable - density.
b is the coefficient of artificial compressibility
8Spatial discretisation
- - finite volume formulation.
- where,
- Qi is the average value of Q in cell i
- Vi is the area of cell i,
- Dlj is the length of side j,
- Fij is the numerical flux across the interface
between cells i and j.
9Spatial discretisation
- Convective fluxes (Fij) are evaluated using Roes
approximate Riemann solver - To ensure second order accuracy, MUSCL
reconstruction is used -
10Time discretisation
- implicit backward Euler scheme with an artificial
time variable t and a linearised RHS.
The resulting block penta-diagonal system is
solved using an approximate LU factorisation.
11Computer Implementation
- A Jameson-type dual time iteration is used to
- eliminate t at each real (outer) iteration and
- recover a divergence free velocity field.
The code vectorises and currently
simulations take about 2 hours per wave to run on
an NEC SX6i deskside supercomputer (!)
12Boundary Conditions
- Seaward boundary a solid moving paddle is used
to generate waves - Atmospheric boundary a constant atmospheric
pressure gradient is applied. Spray and water
passing out of this boundary are lost from the
computation. - Landward boundary a solid wall boundary
condition is used. - Bed and wave energy device modelled using
Cartesian cut cell techniques.
13Cartesian Cut Cell Mesh
- Step 1) Input vertices of solid boundary (and
domain)
14Cartesian Cut Cell Mesh
- Step 2) Overlay Cartesian mesh
15Cartesian Cut Cell Mesh
- Step 3) Identify Cut Cells and compute
- intersection points.
16Cartesian Cut Cell Mesh
- Advantages
- Automatic mesh generation
- Body fitted
- Moving body capability (remesh at each time step)
17Results Wave Paddle Test
- Waves generated by a moving paddle using
AMAZON-SC
Numerical and experimental wave heights
18Results Device Simulation
Simulation of a wave driven rotating vane using
AMAZON-SC
19Conclusions 1
- Initial results have been presented for
non-linear simulation of a rotating vane wave
energy device using a surface capturing method in
a Cartesian cut cell framework - The method can model
- both water and air and their interface
- static and moving boundaries
20Conclusions 2
- Detailed comparisons with small scale
experimental tests are in progress - The numerical model is generic and can be used
to model a wide range of wave energy and other
devices - Project details can be found at
- http//www.owsc.ac.uk/